CENG4480 Lecture 02: Operational Amplifier 1 Bei Yu - PowerPoint PPT Presentation

CENG4480 Lecture 02: Operational Amplifier – 1 Bei Yu byu@cse.cuhk.edu.hk (Latest update: August 19, 2020) Fall 2020 1 / 37

Overview Introduction Op-Amp Preliminaries Op-Amp List 2 / 37

Overview Introduction Op-Amp Preliminaries Op-Amp List 3 / 37

Computer interfacing Introduction To Learn: ◮ how to connect the computer to various physical devices. ◮ Overall interfacing schemes ◮ Analog interface circuits, active filters Some diagrams are taken from references: ◮ [1] S.E. Derenzo, “ Interfacing– A laboratory approach using the microcomputer for instrumentation, data analysis and control ”, Prentice Hall, 1990. ◮ [2] Giorgio Rizzoni, “ Principles and Applications of Electrical Engineering ”, McGraw-Hill, 2005. 3 / 37

Amplifier in Audio System Converting low-voltage sensor signal to a level suitable for driving speaksers. 4 / 37

Typical Data Acquisition and Control System Timer Digital control circuit Sample Sensor filter A/D Op-amp & Hold Computer Mechanical Power D/A device circuit 5 / 37

Analog Interface Example 1 Audio recording systems ◮ Audio recording systems ◮ Audio signal is 20–20KHz ◮ Sampling at 40KHz, 16-bit is Hi-Fi ◮ Stereo ADC requires to sample at 80KHz. ◮ Calculate storage requirement for one hour? ◮ Audio recording standards: Audio CD; Mini-disk MD; MP3 6 / 37

Analog Interface Example 2 Analog hand held controller (a) PS5 (b) Wii (c) Driving wheel 7 / 37

Operational Amplifier (Op-Amp) ◮ Why use op amp? ◮ What kinds of inputs/outputs do you want? ◮ What frequency responses do you want? 8 / 37

Direct Current (DC) amplifier ◮ Example: use power op amp (or transistor) to control the DC motor operation. ◮ Need to maintain the output voltage at a certain level for a long time. ◮ All DC (biased) levels must be designed accurately . ◮ Circuit design is more difficult. DC Op- Load: Source amp DC motor 9 / 37

Biasing Biasing in electronics The method of establishing predetermined voltages or currents at various points of an electronic circuit for the purpose of establishing proper operating conditions in electronic components https://en.wikipedia.org/wiki/Biasing 10 / 37

Alternating Current (AC) amplifier ◮ Example: Microphone amplifier, signal is AC and is changing at a certain frequency range. ◮ Current is alternating not stable. ◮ Use capacitors to connect different stages ◮ So no need to consider biasing problems. AC Op- Load Source amp 11 / 37

Overview Introduction Op-Amp Preliminaries Op-Amp List 12 / 37

Amplifier A circuit where the output signal power is greater than the input signal power. Otherwise is referred as an attenuator . 12 / 37

Black-Box to Consider Circuit Effect ◮ Without examining actual operation (thousands of elements) ◮ Z in : input impedance (a.k.a. R in ) 13 / 37

Voltage gain A A = V out V in ◮ Usually voltage gain may be either very large or very small ◮ Invonvenient to express as a simple ratio ◮ Therefore, decibel (dB): Voltage gain in dB V out A = 20 · log 10 V in 14 / 37

Question: Voltage Gain V in = 20 mV, V out = 500 mV. Calculate the voltage gain in dB. 15 / 37

Operational amplifier circuit diagram 16 / 37

Simplified circuit symbol 2 _ V - 6 LM741 V 0 =A(V + -V - ) V + + 3 ◮ Ideal difference amplifier ◮ (+): noninverting input ◮ (-): inverting input ◮ A : open-loop voltage gain (order of 10 5 to 10 7 ) 17 / 37

R in & R out 2 _ V - 6 LM741 V 0 =A(V + -V - ) V + + 3 ◮ R in : input impedance (High) ◮ R out : output impedance (Low) 18 / 37

Why prefer High R in , Low R out ? Stage1(sensor) Stage 2 Vout1 Rin2 Vin2 Rout1 Is equivelent to: Vin2 Vout1 Rout1 Rin2 19 / 37

Why prefer High R in , Low R out ? Stage1(sensor) Stage 2 Vout1 Rin2 Vin2 Rout1 Is equivelent to: Vin2 Vout1 Rout1 Rin2 To maximize V in 2 R in 2 V in 2 = V out 1 · R out 1 + R in 2 19 / 37

Open-loop & Closed-loop ◮ Open-loop gain ◮ Closed-loop gain Feedback connection The effect of the feedback connection from output to inverting input is to force the voltage at the inverting input to be equal to that at the noninverting input. “Note that closing the feedback loop turns a generally useless amplifier (the gain is too high!) into a very useful one (the gain is just right)!” 20 / 37

Ideal Op-Amp Rules Rule 1 No current flows in or out of the inputs Rule 2 The Op-Amp tries to keep the inputs the same voltage * Rule 2 is only for negtive feedback op-amp 21 / 37

Ideal Op-Amp v.s. Real Op-Amp Open-Loop Gain A Ideal: Infinite, thus V + = V − Real: Typical range (20,000, 200,000), thus V out = A ( V + − V − ) Input Impedance Ideal: Infinite. Since Z in = V in , zero input current I in Real: No such rule. Bandwidth Ideal: Infinite Bandwidth Real: Gain-Bandwidth product (GB). 22 / 37

Gain-Bandwidth Product ◮ Fixed gain-bandwidth product for any given amplifier ◮ Define bandwidth as the frequency range over which the voltage gain of the amplifier is above 70.7% or -3dB of its maximum output value 23 / 37

Slew Rate Limit Slew Rate Slew rate = | dv ( t ) dt | 24 / 37

Overview Introduction Op-Amp Preliminaries Op-Amp List 25 / 37

Voltage follower V 1 + V 0 A _ ◮ Unit voltage gain ◮ Output V 0 = V 1 ◮ high current gain, high input impedance In real op-amp V 0 = A ( V 1 − V 0 ) ⇒ V 0 = V 1 A 1 + A ≈ V 1 25 / 37

Non-inverting Amplifier V1 + A V0 Input _ R2 Output V2 R1 ◮ R in : High input impedance In real op-amp V 0 = A ( V 1 − V 2 ) and V 2 R 1 = R 1 + R 2 V 0 R 1 + ( R 1 + R 2 ) / A ≈ R 1 + R 2 R 1 + R 2 ⇒ V 0 = V 1 R 1 26 / 37

Question: Non-inverting Amplifier Gain V1 + A V0 Input _ R2 Output V2 R1 Calculate V 0 = V 1 27 / 37

Current to Voltage Converter R I _ V 0 A + V 0 = - I · R 28 / 37

Inverting Amplifier Virtual-ground,V2 R 2 Output _ V1 R 1 V0 A Input + Because of Kirchhoff’s circuit laws, i 1 + i 2 = i − = 0 In real op-amp V 0 = A ( 0 − V 2 ) and V 2 − V 1 = V 0 − V 2 R 1 R 2 ⇒ R 1 ( V 0 + V 0 A ) = − R 2 ( V 0 A + V 1 ) ⇒ V 0 ≈ − R 2 V 1 R 1 29 / 37

Inverting Amplifier Virtual-ground,V2 R 2 Output _ V1 R 1 V0 A Input + ◮ R in = R 1 ◮ Gain ( G ) = − R 2 R 1 30 / 37

Inverting Amplifier Virtual-ground,V2 R 2 Output _ V1 R 1 V0 A Input + ◮ R in = R 1 ◮ Gain ( G ) = − R 2 R 1 Question: How to increase input impedance? 30 / 37

Summing Amplifier R V 1 R 1 _ V 2 R 2 V0 I 1 +I 2 +I 3 + Output V 3 R 3 Inputs V 0 = − R · { V 1 + V 2 + V 3 } R 1 R 2 R 3 31 / 37

Differential Amplifier R 2 _ R 1 V 1 V 0 A Input V 2 Output + R 1 R 2 ◮ Calculate the difference between V 1 and V 2 ◮ Can control gain 32 / 37

Question: Differential Amplifier Gain R 2 _ R 1 V 1 V 0 A Input V 2 Output + R 1 R 2 Calculate V 0 = 33 / 37

Question: Differential Amplifier Gain R 2 _ R 1 V 1 V 0 A Input V 2 Output + R 1 R 2 Calculate V 0 = 33 / 37

Instrumental Amplifier ◮ To make a better DC amplifier from op-amps ◮ combine 2 noninverting amplifier & 1 differential amplifier 34 / 37

Instrumental Amplifier (cont.) v1’ v2’ Solution 1: ◮ For each non-inverting amplifier: A = 1 + 2 R 2 R 1 ◮ Connecting to differential amplifier: V out = R F R ( v ′ 2 − v ′ 1 ) = R F R ( 1 + 2 R 2 )( v 2 − v 1 ) R 1 35 / 37

Instrumental Amplifier (cont.) v1’ v2’ Solution 2: ◮ By rule 2, two input voltages are the same, thus = v ′ 2 − v ′ v 2 − v 1 1 2 R 1 + R R 1 = ( 1 + 2 R 1 ◮ Therefore: v ′ 2 − v ′ R )( v 2 − v 1 ) 36 / 37

Comparing Amplifiers Op Amp Inv. Amp Noninv. Amp Diff. Amp Instr. Amp High R in � X � X � Diff Input � X X � � Define Gain X � � � � 37 / 37